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Updated: Sep 11, 2025

Synthesis and Operation of Fluorescent-core Microcavities for Refractometric Sensing
Published on: March 13, 2013
Baseline-free wavelength modulation spectroscopy based on cepstral analysis
None:
This paper demonstrates what we believe to be a new WMS m-FID technique based on cepstral analysis, incorporating wavelength modulation spectroscopy (WMS) with a modified form of the time-domain molecular free-induction decay (m-FID) signal. Detailed theoretical framework of the WMS m-FID technique, as well as the fitting routine, has been investigated. The proposed WMS m-FID technique is first validated through a static CO gas cell experiment using the CO R(9) absorption line near 2179.7719 cm-1. The fitting error between the measured and best-fit m-FID signals is less than 1.0 %, with integrated absorbance area of relative uncertainty 0.17 %. Time-resolved measurements of CO over a 6-second purge period demonstrate the reliability and robustness of the proposed WMS m-FID approach in comparison with direct absorption spectroscopy (DAS) and WMS-2f/1f techniques. The demonstration of the proposed WMS m-FID approach is further carried out in a premixed CH4/Air laminar flame of a flat-flame burner. The relative fitting residuals between the measured and best-fit m-FID signals remain below 4.0 %, yielding T = 1763 K and XH2O=16.58 % at HAB = 7 mm, with a temperature uncertainty of 30 K and absolute H2O concentration uncertainty of 0.65 %. The average temperature difference between the WMS m-FID and WMS-2f/1f techniques is within 18.0 K (<1.0 % relative), and the H2O concentration difference is within 0.4 % (<2.6 % relative). Additionally, the proposed WMS m-FID technique significantly improves computational efficiency, enabling 22-fold acceleration compared to the time-consuming spectral-fitting routine in standard WMS-2f/1f techniques. Finally, a strictly baseline-free CO measurement is achieved by directly fitting the m-FID signal of the measured transmitted intensity beyond the 3rd-order peak (τ ≥ ~5.7 ns) and the 4th-order peak (τ ≥ ~7.7 ns), with deviations of 2.7 % and 4.4 % from the entire m-FID signal fitting, respectively. Both the static gas-cell and high-temperature flat-flame demonstrations indicate that the proposed WMS m-FID technique enables quantitative, accurate, and baseline-free measurements. It is envisioned that the WMS m-FID technique can be an effective solution for achieving baseline-free, quantitative, in situ monitoring in practical combustion environments.
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